Since the hinge C is in equilibrium, the sum of the forces applied to it is zero.
Writing the projections of the forces (Fig. 182) acting on the hinge C on the axis perpendicular to AC, we obtain
where mhin is the mass of the hinge. Similarly, from the equilibrium condition for the hinge D and from the condition that the middle rod is horizontal, we obtain
Solving Eqs. (1) and (2) together, we find that
Thus, the minimum force Fmin for which the middle rod retains its horizontal position is
and directed at right angles to the rod BD.